In this paper, a nonstatic point, nonlocal Dirac electron model (DEM) is derived making only one assumption: the Dirac equation (DE) is an accurate description of the free electron. In the DEM, the center of charge (CoC) coordinate operator oscillates very rapidly around the “fictitious” center of mass (CoM) coordinate operator with the Zitterbewegung period of ~1.5x10-21 s. A major objection to any distributed electron charge distribution is the proof that electron cannot have its charge distributed in two or more points at the same time [V. F. Weisskopf, Phys. Rev. 56, 72 (1939); Rev. Mod. Phys. 21, 2 (1949)] without creating infinite self energy. The DEM is not subject to this limitation, however, since the electron charge is located at only one point (the CoC) at any one time, and this limitation does not apply. The electron creates the illusion that the nonrelativistic electron charge is a static point charge located at its CoM with “intrinsic” spin and magnetic moment. In fact, the DEM shows that the electron’s CoC is in rapid oscillation about its CoM, which creates a charge shell and magnetic moment over time that defines the intrinsic electron properties deterministically with DE quantum position and velocity operators. The DEM defines a nonrelativistic electron whose electric field “seems like” it originates from a static point located at the electrons CoM. The nonrelativistic electron’s magnetic field seems like it is generated from on intrinsic point magnetic dipole located at the electron’s CoM, but an experiment is described in this paper to test the DEM predictions. The assumption that an electron is located at a single static point leads to infinite answers for electron self energy in classical electrodynamics, quantum mechanics, and quantum electrodynamics (QED), which is an absurd result. In the DEM, where the CoC position operator oscillates rapidly about its CoM, the electron self energy is finite in the rest frame, but is impossible to measure since one cannot turn the electron’s charge off to measure its bare mass. This paper presents a very clear experiment, where the differences in the electron’s electromagnetic (EM) field magnitude perpendicular to its CoM velocity is much greater for the static point electron than for the DEM dynamic point electron as the CoM speed approaches the speed of light, c. The static point to DEM ratio of the electron’s EM field magnitudes becomes infinite as the CoM speed approaches c. At very high CoM speeds, where pair production and annihilation effects are significant, the electron’s EM magnitude perpendicular to the CoM velocity will be even lower than the DEM estimate, since the effective electron charge is spatially spread out even more than the DEM predicts. The electron’s CoC operator is derived directly from the DE with no additional assumptions and oscillates as a set of three one dimensional harmonic oscillators. The Dirac electron does NOT have a spatial structure with distributed charge, but is NOT a single, static point either. The Dirac electron CoC coordinate operators can be described as a stable harmonic oscillation in the vacuum. The electron CoC operator is located on a spherical shell in the rest frame with a radius on the order of its Compton wavelength. In the nonrest frame, the electron’s CoC operator is located on an oblate spheroid, flattened by the special relativity factor γ2=1/(1-ν2/c2) in the direction of its CoM velocity and by c in the directions perpendicular to its COM velocity. In the DEM, the electron self energy is finite, and the QED structureless electron properties [V. F. Weisskopf, Phys. Rev. 56, 72 (1939); V. F. Weisskopf, Rev.Mod. Phys. 21, 2 (1949)], such as the Lamb shift and anomalous magnetic moment, are not impacted at all by the DEM.